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kondaur
2 months ago
10

Oceanographers use submerged sonar systems, towed by a cable from a ship, to map the ocean floor. In addition to their downward

weight, there are buoyant forces and forces from the flowing water that allow them to travel in a horizontal path. One such submersible has a cross section area of 1.3m2 , a drag coeffecient of 1.2, and when towed at 4.3 m/s, the tow cable makes an angle of 30 degrees with the horizontal. What is the tension in the cable? Take the water density to be 1000 kg / m3
Physics
1 answer:
Yuliya22 [3.3K]2 months ago
7 0
The tension exerted in the cable amounts to T = 16653.32 N. Parameters: Cross section area A = 1.3 m² Drag coefficient CD = 1.2 Velocity V = 4.3 m/s The angle formed by the cable with the horizontal is 30 degrees. Density defined as follows: The drag force FD is determined by the equation: FD = (1/2) * ρ * V² * A * CD Calculating the drag force yields 14422.2 N acting opposite to motion. Given the cable's angle of 30 degrees with horizontal, the horizontal component contributes to the drag force calculation: T * cos(30) = F_D Thus, T = 16653.32 N.
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Newton’s law of cooling states that dx dt = −k(x−A) where x is the temperature,t is time, A is the ambient temperature, and k &g
Maru [3345]

Answer:

a) X= kA_o\dfrac{1}{k^2+\omega^2}\left ( kcos\omega t+\omega sin\omega t \right )+Ce^{-kt}

b) D does not influence the long-term results.

Explanation:

Given that

\dfrac{dx}{dt}=-k(x-A)

A = A0 cos(ωt)

\dfrac{dx}{dt}=-k(x-A_o cos(\omega t))

\dfrac{dx}{dt}+kx=kA_o cos(\omega t)This is a linear equation hence the integration factor, I

I=e^{\int kdt}

I=e^{kt}Now using the characteristics of linear equations

e^{kt} X=\int e^{kt} kA_o cos(\omega t) dt +C

e^{kt} X= kA_o \dfrac{e^{kt}}{k^2+\omega^2}\left ( kcos\omega t+\omega sin\omega t \right )+C

b) At t= 0

X= kA_o\dfrac{1}{k^2+\omega^2}\left ( kcos\omega t+\omega sin\omega t \right )+Ce^{-kt}

Thus, the initial condition

does not affect the long-term outcome.

X(0)=\dfrac{k^2A_o}{\omega^2+k^2}+C

5 0
2 months ago
A 1/10th scale model of an airplane is tested in a wind tunnel. The reynolds number of the model is the same as that of the full
Yuliya22 [3333]

Answer:

the airspeed of a full-sized aircraft

7 0
2 months ago
A team of engineering students is testing their newly designed 200 kg raft in the pool where the diving team practices. The raft
Sav [3153]

Answer:

The water level increases more when the cube is above the raft before it sinks.

Explanation:

The principle involved is based on Archimedes' theory, which states that immersing an object in water will raise the initial water level. This means that the height of the water in the container increases. The increase in water volume corresponds to the volume of the submerged object.

We can consider two scenarios: when the steel cube rests on the raft and when it settles at the pool's bottom.

When the cube rests at the pool’s bottom, the volume will indeed rise, and we can ascertain this using the cube's volume.

Vc = 0.45*0.45*0.45 = 0.0911 [m^3]

When an object floats, it's because the densities of the object and water are in equilibrium.

Ro_{H2O}=R_{c+r}\\where:\\Ro_{H2O}= water density = 1000 [kg/m^3]\\Ro_{c+r}= combined density cube + raft [kg/m^3]

The formula for density is:

Ro = m/V

where:

m= mass [kg]

V = volume [m^3]

The buoyant force can be calculated with this equation:

F_{B}=W=Ro_{H20}*g*Vs\\W = (200+730)*9.81\\W=9123.3[N]\\\\9123=1000*9.81*Vs\\Vs = 0.93 [m^3]

Vs > Vc indicates that the combined volume of the raft and the cube exceeds that of the cube alone resting at the bottom of the pool. Hence, when the cube is positioned above the raft, the water level rises more before it becomes submerged.

7 0
3 months ago
Classes are canceled due to snow, so you take advantage of the extra time to conduct some physics experiments. You fasten a larg
Maru [3345]

1) 9.18 s

During the initial phase, the rocket accelerates at

a_1=13.5 m/s^2

over a time interval of

t_1=3.50 s

The final velocity after this period is found using the SUVAT formula:

v_1=u+a_1t_1

with initial velocity u = 0. Substituting a1 and t1 gives:

v_1=(13.5)(3.50)=47.3 m/s

Afterward, the rocket decelerates uniformly at

a_2 = -5.15 m/s^2

until it stops, meaning the final velocity is

v_2 = 0

Again using the SUVAT formula,

v_2 = v_1 + a_2 t_2

and knowing v_1 = 47.3 m/s, solve for t2, the time until the rocket halts:

t_2 = -\frac{v_1}{a_2}=-\frac{47.3}{5.15}=9.18 s

2) 299.9 m

Calculate distances covered in both phases.

Distance in the first phase:

d_1 = ut_1 + \frac{1}{2}a_1 t_1^2

Substituting values from part 1,

d_1 = 0 + \frac{1}{2}(13.5) (3.50)^2=82.7 m

Distance in the deceleration phase:

d_2= v_1 t_2 + \frac{1}{2}a_2 t_2^2

Substituting known values,

d_2 = (47.3)(9.18) + \frac{1}{2}(-5.15) (9.18)^2=217.2 m

Total distance traveled is

d = 82.7 m + 217.2 m = 299.9 m

6 0
3 months ago
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